(19)
(11) EP 0 856 752 B1

(12) EUROPEAN PATENT SPECIFICATION

(45) Mention of the grant of the patent:
09.05.2001 Bulletin 2001/19

(21) Application number: 98300403.7

(22) Date of filing: 20.01.1998
(51) International Patent Classification (IPC)7G02B 6/16, G02F 1/01

(54)

Magnetically tunable optical fiber gratings

Magnetisch abstimmbare optische Fasergitter

Réseaux de guides d'onde optiques magnétiquement accordables


(84) Designated Contracting States:
DE GB

(30) Priority: 29.01.1997 US 791081

(43) Date of publication of application:
05.08.1998 Bulletin 1998/32

(73) Proprietor: LUCENT TECHNOLOGIES INC.
Murray Hill, New Jersey 07974-0636 (US)

(72) Inventors:
  • Jin, Sungho
    Millington, NJ 07946 (US)
  • Strasser, Thomas A.
    Chatham, NJ 07928 (US)
  • Lemaire, Paul Joseph
    Madison, NJ 07940 (US)

(74) Representative: Johnston, Kenneth Graham et al
Lucent Technologies (UK) Ltd, 5 Mornington Road
Woodford Green Essex, IG8 OTU
Woodford Green Essex, IG8 OTU (GB)


(56) References cited: : 
WO-A-95/30926
US-A- 5 394 488
US-A- 4 996 692
   
  • X.-Z. LIN ET AL.: "Electrically tunable singlemode fibre Bragg reflective filter" ELECTRONICS LETTERS, vol. 30, no. 11, 26 May 1994, pages 887-888, XP002063592
  • QUETEL L ET AL: "PROGRAMMABLE FIBER GRATING BASED WAVELENGTH DEMULTIPLEXER" OPTICAL FIBER COMMUNICATION (OFC) 1996, SAN JOSE, FEB. 25 - MAR. 1, 1996, vol. VOL. 2, no. CONG. 19, 25 February 1996, OPTICAL SOCIETY OF AMERICA, page 120/121 XP000620997
   
Note: Within nine months from the publication of the mention of the grant of the European patent, any person may give notice to the European Patent Office of opposition to the European patent granted. Notice of opposition shall be filed in a written reasoned statement. It shall not be deemed to have been filed until the opposition fee has been paid. (Art. 99(1) European Patent Convention).


Description

FIELD OF THE INVENTION



[0001] The present invention relates to optical fiber gratings and, in particular, to fiber gratings tunable by magnetic force.

BACKGROUND OF THE INVENTION



[0002] Optical fibers are key components in modern telecommunications systems. Optical fibers are thin strands of glass capable of transmitting an optical signal containing a large amount of information over long distances with very low loss. In essence, an optical fiber is a small diameter waveguide characterized by a core with a first index of refraction surrounded by a cladding having a second (lower) index of refraction. Light rays which impinge upon the core at an angle less than a critical acceptance angle undergo total internal reflection within the fiber core. These rays are guided along the axis of the fiber with minimum attenuation. Typical optical fibers are made of high purity silica with minor concentrations of dopants to control the index of refraction.

[0003] Optical fiber Bragg gratings are important elements for selectively controlling specific wavelengths of light within an optical fiber. A typical Bragg grating comprises a length of optical fiber including a plurality of perturbations in the index of refraction substantially equally spaced along the fiber length. These perturbations selectively reflect light of wavelength λ equal to twice the spacing Λ between successive perturbations, i.e. λ = 2neffΛ, where λ is the vacuum wavelength and neff is the effective refractive index of the propagating mode. The remaining wavelengths pass essentially unimpeded. Such Bragg gratings have found use in a variety of applications including filtering, stabilization of semiconductor lasers, reflection of fiber amplifier pump energy, and compensation for fiber dispersion.

[0004] Conventional fiber Bragg gratings are conveniently fabricated by providing fiber with one or more dopants sensitive to ultraviolet light, such as fibers having cores doped with germanium oxide, and exposing the fiber at periodic intervals to high intensity ultraviolet light from an excimer laser. The ultraviolet light interacts with the photosensitive dopant to produce long-term perturbations in the local index of refraction. The appropriate periodic spacing of perturbations to achieve a conventional grating can be obtained by use of a physical mask, a phase mask, or a pair of interfering beams.

[0005] A difficulty with conventional fiber gratings is that they filter only a fixed wavelength. Each grating selectively reflects only light in a narrow bandwidth centered around λ = 2neffΛ. However in many applications, such as multiplexing, it is desirable to have a tunable grating whose wavelength response can be controllably altered.

[0006] One attempt to make a tunable fiber grating uses a piezoelectric element to strain the grating. See Quetel et al., 1996 Technical Digest Series, Conf. on Optical Fiber Communication, San Jose, Calif., Feb. 25- March 1, 1996, Vol. 2, p. 120, paper No. WF6. The difficulty with this approach is that the strain produced by piezoelectric actuation is relatively small, limiting the tuning range of the device. Moreover, it requires a continuous application of relatively high voltage, e.g., approximately 100 volts for 1 nm strain. A further attempt to make a tunable fibre grating uses a magnetostrictive substrate to strain the grating. See "Electrically tunable singlemode fibre Bragg reflective filter" by X.-Z. Lin et al., Electr. Lett., 26th May 1994, Vol. 30, No. 11, pp. 887-8. A related device is described in WO 95/30926 A which describes a device in which the portion of an optical fibre containing a grating is glued to a glass base. Tension is applied to this portion by attaching weights to a cord which is separately glued to the fibre at the end of the cladding that is closest to the weight. Accordingly, there is a need for a tunable fiber grating having an enhanced tuning range and no requirement for continuous power.

SUMMARY OF THE INVENTION



[0007] In accordance with the invention as defined in claim 1, a tunable fiber grating comprises a fiber grating secured between a pair of magnets so that magnetic force (repulsive or attractive) applied to the magnets is transmitted to the grating. An electromagnet is disposed adjacent the magnets for applying the field to magnetize them. Control of the current applied to the electromagnet permits control of the force transmitted to the fiber grating and, thus, control of the grating strain, spacing and reflection frequency. In a preferred embodiment the electromagnet is actuated to produce magnetic pulses which control the remanent force between the two magnets, eliminating the need for continuous power. An add/drop multiplexer employing the tunable gratings is described.

BRIEF DESCRIPTION OF THE DRAWINGS



[0008] The advantages, nature and additional features of the invention will appear more fully upon consideration of the illustrative embodiments described in the accompanying drawings. In the drawings:

FIGS. 1(a) and 1(b) schematically illustrate tunable fiber gratings using magnetic strain tuning;

FIG. 2 is a schematic graphical illustration useful for describing the programmability of remanent fiber strain by adjusting applied magnetic field pulses;

FIG. 3 is a schematic graphical illustration showing bistable magnetically induced fiber strain;

FIG. 4 is a flow diagram illustrating a preferred method for making and using the devices of Figs. 1(a) and 1(b).

FIGS. 5-8 schematically illustrate various alternative embodiments of the Fig. 1 device; and

FIG. 9 illustrates an N-channel optical ADD/DROP multiplexing device using a tunable fiber grating.

It is to be understood that these drawings are for purposes of illustrating the concepts of the invention and are not to scale. The same reference numerals are used to designate similar elements throughout the drawings.

DETAILED DESCRIPTION



[0009] Referring to the drawings, Fig. 1(a) schematically illustrates a tunable fiber grating 10 comprising a length of optical fiber 11 including a grating 12 of index perturbations 13. The fiber in the region of the grating is secured, as by bonding or mechanical attachment, between a pair of magnets 14, 15 for transmitting force between the magnets to the grating 12. The magnets can be permanent magnets or, less preferably, bodies of soft magnetic material such as iron. The magnets can conveniently be cylinders each concentrically surrounding the fiber. One or more electromagnets (solenoids) 16, 17 are disposed adjacent the magnets 14, 15 for providing a controllable magnetic field between them.

[0010] The fiber grating is firmly attached to the magnets, either by mechanical clamping or by bonding, as with epoxy or solder. In the use of solder, the fiber surface is desirably coated with a metal layer to improve solder bond strength. Here the adhesive is shown as bonding layers 18. Where, as illustrated, similar magnetic poles are adjacent (S adjacent S), the field forces the magnets apart along direction of the fiber grating. Alternatively, as shown in Fig. 1(b) magnets 14, 15 can be oriented so that opposite poles are adjacent (S adjacent N, and the field from electromagnets 16, 17 will produce a compressive strain on the grating. In this case, a fiber retainer tube (capillary tube) 19 is preferably provided to avoid localized fiber deflection.

[0011] On operation, the force transmitted from the magnets to the grating produces a strain which changes the wavelength response of the grating. When the fiber grating is stretched or compressed, e.g., 1% in length (ε=Δl/l=0.01), the grating periodicity Λ will also change. However, the resonating Bragg reflection wavelength λ will not change by exactly 1%, since the interatomic distance in the glass is also affected by the elastic strain and as a result the refractive index n is altered. This strain effect on refractive index can be represented by a photoelastic constant Pε which is typically about 0.22 for the SiO2 fiber. The wavelength change induced by the magnetically applied strain ε (ε=Δl/l) is thus expressed as Δλ/λ=(Δ l/l)(1-Pε)=ε(1-Pε). The strain ε is determined by the applied stress (σ) and the elastic modulus (E), ε=σ/E, and the stress on the fiber is the force (F) divided by the cross-sectional area (πr2) where r is the radius of the fiber grating. Rearranging these equations, Δλ/λ=(F/πr2)(1/E)(1-Pε). For example, for λ=1550 nm, F=1200 gm gives a shift in wavelength Δλ=16.01 nm or about 1% change. For a wavelength-division-multiplex channel spacing of 0.8 nm, this induced Δλ is sufficient to alter the filtered wavelength over a 20 channel span.

[0012] An important advantage of this device is that continuous power is not required to maintain a wavelength shift. FIG. 2 is a schematic plot of the strain ε in the fiber as a function of the applied magnetic field H. There is a left-over remanent strain after the field is removed. The remanent strains for the field strengths H1, H2, and H3 are ε1, ε2, and ε3, respectively. The magnitude of this remanent strain depends on the magnitude of the applied field, and it is therefore programmable by selecting a proper field strength. To change ε to a higher value, the applied H in a subsequent pulse is raised by increasing the pulse current in the solenoid. To lower ε, a demagnetizing AC current with a diminishing amplitude is applied to partially demagnetize the magnets and the new magnetizing DC current pulse is applied to achieve the new desired remanent magnetization state.

[0013] Instead of a continuously tunable grating, the device can be bistably tuned between two wavelengths. A magnetic material with strong anistropy and an axis of magnetization aligned parallel to the optical fiber axis has a square hysteresis loop. See Jin et al., IEEE Trans. Magn., MAG-23, No., 5, p. 3187 (1987). FIG. 3 is a plot of the strain ε vs applied field H for a cyclic variation showing a square hysteresis loop. The use of deformation aged Fe-Cr-Co alloys is partially preferred for magnets exhibiting such a loop shape.

[0014] With magnets exhibiting a square hysteresis loop, one can make bistable strain devices that switch between two wavelengths: e.g. a zero strain Bragg reflection wavelength λ0 and a saturation-strained reflection wavelength λ1. λ0 is achieved by applying an AC demagnetizing field. λ1 is achieved by a DC pulse current sufficient to saturate the magnets. The advantage of the bistable device is reduced sensitivity to the applied current or to stray magnetic fields.

[0015] Fig. 4 is a flow diagram illustrating the steps in the preferred process for making the tunable optical fiber grating of Figs 1(a) and 1(b). The first step shown in block A is to provide an optical fiber grating having a desired Bragg reflection wavelength for dropping or adding a wavelength component. For example, for a median light beam wavelength of 1550 nm, the grating periodicity Λ in a SiO2 based fiber (with a refractive index n~1.45) is 500 nm. The length of each optical fiber grating to be incorporated into the grating assembly is typically in the range of 5 mm to 100 mm and preferably in the range of 10-50 mm. For the short fiber grating, the region of the regular fiber outside the grating can be used for attachment to the magnetic components.

[0016] The next step shown as block B is to provide magnetic components to be attached to the fiber grating. At least two magnetic components, each either a single piece or an aggregate, are needed. They are oriented with their magnetic poles parallel to the axis of the fiber grating. At least a portion of each magnetic component should be semi-hard or permanent with a remanent magnetization. Yet its strength should be reprogrammable by altering the applied magnetic field. When the two magnets have the same magnetic poles facing each other, e.g., the south against the south pole, they repel each other. The fiber grating attached to them is under tensile stress, with the tensile elastic strain ε proportionally increasing as the stress σ is increased (ε=σ/E where the elastic modulus E=10.5×106 psi for silica glass). When the two facing poles are different, i.e., south against north, the two magnets are attracted to each other by magnetic force, and the fiber grating is under compressive stress. When a compressive stress is used, undesirable buckling or deflection of the fiber grating should be prevented or minimized, as by the use of a capillary tube restricting the off-axis movement of fiber grating. A suitable low-friction coating such as a fluorocarbon or diamond may optionally be used for easy sliding of the fiber in the tube.

[0017] The third step (block C of Fig. 4) is to align and attach the two magnetic components onto the fiber. The magnets can have a cylindrical configuration or a blocky configuration. In the exemplary embodiment of Fig. 1 both ends of the fiber grating (areas outside the active Bragg reflection region) are firmly attached to each of the two tunable magnet components. To assure a strong bonding and minimize strain relaxation at the interface of the fiber and the magnet components, the use of mechanically strong, non-thermoplastic adhesive or a solder with a relatively high melting point and high mechanical strength is desired. The fiber surface to be attached is desirably coated with a metal layer to improve the solder bond strength.

[0018] For maximizing the magnetic force for a given volume of the magnet, the air gap between the facing poles should be very small. The magnetic force decreases as the gap is increased. The preferred gap is less than about 0.200", and more preferably, less than 0.050".

[0019] The preferred magnet materials are those whose magnetic properties are modifiable by a pulse magnetic field. Some examples of suitable magnets are Fe-Cr-Co, Fe-Al-Ni-Co (Alnico), Cu-Ni-Fe (Cunife), Co-Fe-V (Vicalloy), specially-processed, low-coercivity (He) rare earth cobalt (Sm-Co) or Nd-Fe-B magnets, and Ba-ferrite or Sr-ferrite magnets. The desired range of the coercivity is typically below 3000 Oe and preferably below 1000 Oe for the ease of programming by re-magnetization using solenoid pulse field. The coercivity is typically above 50 Oe and preferably above 200 Oe for maintaining the stability of the remanent magnetization and also for stability against demagnetization due to stray magnetic fields. Mechanically ductile and easily machineable magnet alloys such as Fe-Cr-Co, Cu-Ni-Fe, Co-Fe-V are particularly desirable for shaping into desired geometry. Stable permanent magnets with high coercive forces, such as Sm-Co or Nd-Fe-B are less desirable (unless modified to exhibit lower coercive forces) because of the difficulty in reprogramming the remanent magnetization using low magnetic field. These stable magnets, however, can be used for supplying a basis (or bias) field, in combination with programmable magnets.

[0020] The next steps in FIG. 4 (Steps D and E) are to add at least one solenoid winding around the magnetic components and to apply a programmed pulse field to adjust the remanent magnetization in the magnets. This adjustment alters the force and the strain on the fiber grating. A constant DC field, instead of a pulse field can also be used, but the use of a DC pulse field is preferred so that a constant supply of electrical current to the solenoid is avoided. The desired duration or speed of the pulse field is typically in the range of 1-10-8 seconds, preferably 1-10-6 seconds and even more preferably 10-1-10-4 seconds. For a thick magnet geometry, the use of pulses that are too fast is not desirable because of the eddy current loss. The shape of the current pulse can be rectangular, rectified sinusoidal or irregular as long as the maximum field needed for a magnetization to the pre-determined remanence is accomplished.

[0021] FIG. 5(a) through 5(e), shows the shapes of a variety of useful magnetic components 14, 15. The magnets can be cylinders with a center hole (FIG. 5(a)), round or block-like, two-piece magnets (FIG. 5(b)-(d)), or substrate-like magnets (FIG. 5(e)). The two piece magnet configuration with center axis aligning grooves is preferred because of its convenience for device assembly.

[0022] While the device configuration illustrated in FIG. 1 is one of the simplest, other embodiments are depicted in FIGS. 6-8. In the embodiment of FIG. 6(a), the two programmable magnets 14, 15 and the accompanying solenoids 16, 17 are shorter than in FIG. 1, but are still facing each other with a small air gap. The magnets are secured to the fiber through extensions of nonmagnetic material 60 such as glass, aluminum, copper, or stainless steel. This configuration is viable when the magnitude of desired wavelength tuning is not extensive, and when the short magnets provide sufficient magnetic force. In the alternative embodiment of FIG. 6(b), small but strong, high-coercivity magnets 61, 62 (such as Nd-Fe-B or Sm-Co) which provide the bias field are combined with low-coercivity programmable magnets 14, 15. The high coercivity magnets are secured to the fiber through extensions of low coercivity magnetic material. It is also possible, as illustrated in Fig. 6(c) to tune the programmable magnets 14, 15 through field-amplifying soft magnets 63, 64 (such as iron, Ni-Fe permalloy, Si-steel, etc) for the purpose of obtaining a higher magnetizing field using a small electrical current in the solenoid.

[0023] Fig. 7 illustrates yet another embodiment where a substrate 70 allows a tensile stress (instead of compressive stress) to be applied to the fiber grating using magnetic attraction between unlike poles. This configuration is convenient in that a tensile force on fiber eliminates the need to guard against possible fiber buckling. Also, an attractive magnetic force maintains the axial alignment of magnets with a minimal need to guard against lateral force. In this configuration, one end of the fiber grating 12A is firmly fixed onto the substrate. The other end of the grating is 12B fixed onto the leading end of the programmable magnet 14. Another magnet 15 with a magnetically attractive arrangement is attached onto the substrate further away from the leading end of the programmable magnet. Thus one magnet is secured to the fiber through a nonmagnetic substrate.

[0024] The smaller magnet 15 can either be a programmable magnet or a non-programmable magnet that contributes to the overall magnetic attractive force. In the latter case, very strong magnets, such as, Sm-Co or Nd-Fe-B magnets, can be used. Alternatively, a field amplifying soft magnetic material can be used instead of the strong magnet. If the attachment configuration and locations of fiber-substrate and magnet-fiber bonding are modified, a compressive, instead of tensile, stress on the fiber grating can be produced using a magnetic attraction force.

[0025] FIG. 8 shows an embodiment including a magnetic return path 80 of soft magnetic material employed for reduced leakage flux and maximum utilization of magnetic strength of the magnets with a given volume. The return path extends between opposite poles of magnets 14, 15 respectively..

[0026] The gratings described herein are especially useful in wavelength division multiplexed communications system which employ multiplexer/demultiplexer devices. In such systems, a "trunk" fiber carries optical signal channels at several wavelengths λ1, λ2,...λn and it is desirable to extract a single wavelength channel from the trunk fiber or to add a single wavelength channel onto the trunk. A wide variety of such devices can be made by interconnecting optical circulators and fiber gratings. Typically the channel reflected by the grating is dropped from the trunk fiber or is added to the trunk. Gratings as described herein permit selection at the grating of which channel is dropped or added.

[0027] FIG. 9 schematically illustrates a wavelength division multiplexed (WDM) communications system comprising a transmitter 100, an improved N-channel multiplexer/demultiplexer 101 and a receiver 102, all connected by trunk fiber 11. The input on fiber 11 consists of optical signals at several wavelengths, λ1 to λn.

[0028] The improved multiplexer 101 comprises one or more pairs (here 3 pairs) of circulators. The circulators of each pair are separated by a grating. For example, the first pair of circulators comprises upstream circulator 90A and downstream circulator 90B separated by grating 12A. The second pair is 90C and 90D separated by grating 12C. In each pair, the upstream circulator (90A, 90C, 90E) serves to divert a forward propagating channel that matches the corresponding grating (12A, 12C, 12E) into a corresponding DROP port 91A, 91C, 91E. The downstream circulator (90B, 90D, 90F) similarly serves to insert into fiber 11 signals at ADD ports 92B, 92D, 92F, provided the wavelengths of the signals to be added correspond to the respective gratings 12A, 12C and 12E.

[0029] The device is improved by making any one of these gratings 12A, 12C, 12E tunable as set forth above, and preferably by making each tunable. If the grating is tuned so that it coincides with a different channel, then the different channel can be added or dropped. Moreover, a tunable grating can also perform a DISABLE function. If the grating is tuned between the channels, then the ADD/DROP function is temporarily disabled.

[0030] In alternative embodiments the improved multiplexer can comprise a single pair of circulators with a plurality of tunable gratings disposed between them for performing ADD, DROP or DISABLE functions.

EXAMPLE



[0031] A 32-channel, reconfigurable ADD/DROP system for Wavelength Division Multiplexing is constructed using 32 magnetostatically tunable fiber gratings connected in a series with associated circulators or directional couplers to serve as ADD or DROP ports as schematically illustrated in Fig. 9.

[0032] The nominal (mean) wavelength of the optical signal to be processed is 1550nm, and the signal wavelength channels are separated from one another by a spacing of 0.8 nm producing a center - to - center spacing with a channel width of 0.3nm. The refractive index periodicity (Λ) of each grating is made into a predetermined dimension so that all 32 gratings have their Bragg reflection wavelengths off by a half channel (placed at the mid-channel positions), and hence with no tuning activated, all 32 wavelength signals pass through the ADD/DROP system without being filtered (dropped). If a certain selected group of channels (e.g., Channels #1, #5, and #27) need to be dropped, the magnetostatic tuning devices for those gratings are activated by a magnetic pulse field so as to strain the fiber gratings by 1/2 channel, e.g., Δλ/λ of roughly 0.4 nm/1550nm ≈ 0.025%. The programmable magnet material and the magnitude of the magnetic field applied is predetermined to produce and maintain this amount of remanent strain in the fiber, and to make the channels #1, #5 and #27 Bragg reflected and filtered (dropped). To cancel the DROP operation of a channel, e.g. channel #3, a demagnetizing AC field with gradually decreasing amplitude (e.g. 60 Hz field applied for 2 seconds) is applied to the magnet element to remove the strain on the fiber grating. The ADD operation is performed in a similar manner (e.g. for channels #4, #9, #14 and #23) but with a backward transmission through a circulator and Bragg reflection in the forward direction.

[0033] It is to be understood that the above-described embodiments are illustrative of only a few of the many possible specific embodiments which can represent applications of the invention. Numerous and varied other arrangements can be made by those skilled in the art without departing from the scope of the invention as defined in the appended claims.


Claims

1. A tunable optical fiber grating device comprising:

a length of optical fiber (11) including an optical grating (12) along a portion of its length;

a pair of magnets (14, 15) secured to said fiber on opposite sides of said grating;

an electromagnet (16, 17) for applying a magnetic field to said magnets, thereby inducing force between said magnets and creating strain across said grating.


 
2. A tunable grating device according to claim 1, wherein the magnets of said pair maintain a remanent strain in said grating until deactivation.
 
3. A tunable grating device according to claim 1, including a current source for activating said electromagnet by a DC pulse for producing sufficient remanent magnetization of the magnets of said pair to maintain a remanent strain in said grating.
 
4. A tunable grating device according to claim 1, including a current source for applying a diminishing AC current to said electromagnet for removing remanent magnetization of said pair of magnets.
 
5. A tunable grating device according to claim 1, wherein said magnets are spaced apart with adjacent ends having either opposite magnetic polarity, or the same magnetic polarity.
 
6. A tunable grating device according to claim 1, further comprising a current source for applying a pulsed current to said electromagnet.
 
7. A tunable grating device according to claim 1 wherein the magnets of said pair exhibit a square hysteresis loop for producing a grating device having a bistable wavelength response.
 
8. A tunable grating device according to claim 1, wherein said magnets are secured to said fiber through either a non magnetic extension, or an extension of magnetic material, for example soft magnetic material.
 
9. A tunable grating device according to claim 1, wherein said fiber is secured to one magnet of said pair through a nonmagnetic substrate.
 
10. A tunable grating device according to claim 1 further comprising a flux return path extending between opposite of said pair of magnetic field leakage.
 
11. An optical multiplexer/demultiplexer comprising at least a first and a second optical circulators (90a, 90b) and an optical fiber (12a) grating connecting said first and said second optical circulators, wherein said optical fiber grating is a tunable grating according to claim 1.
 
12. A N-channel optical ADD/DROP multiplexer/demultiplexer comprising a plurality of optical circulators (90a, 90b, 90c,...) and a plurality of optical fiber gratings (12a, 12b, 12c) interconnected by an optical fiber for adding and/or dropping an optical communications channel from said fiber, wherein at least one optical fiber grating is a tunable grating according to claim 1.
 
13. A wave division multiplexed optical communications system comprising: a source (100); an optical trunk fibre (11) for transmitting multiple wavelength optical signal channels from said source; and a multiplexer/demultiplexer, which comprises a device according to claim 1.
 


Ansprüche

1. Abstimmbares faseroptisches Gitterbauelement, das folgendes umfaßt:

ein Stück optische Faser (11) mit einem optischen Gitter (12) entlang einem Teil seiner Länge;

ein Paar von Magneten (14, 15), die auf gegenüberliegenden Seiten des Gitters an der Faser befestigt sind;

einen Elektromagneten (16, 17) zum Anlegen eines Magnetfeldes an die Magnete, wodurch zwischen den Magneten eine Kraft induziert und an dem Gitter eine Verformung erzeugt wird.


 
2. Abstimmbares Gitterbauelement nach Anspruch 1, bei dem die Magnete des Paars bis zu einer Deaktivierung eine remanente Verformung in dem Gitter aufrechterhalten.
 
3. Abstimmbares Gitterbauelement nach Anspruch 1, mit einer Stromquelle zum Aktivieren des Elektromagneten durch einen Gleichstromimpuls zum Erzeugen einer ausreichenden remanenten Magnetisierung der Magnete des Paars, um eine remanente Verformung in dem Gitter aufrechtzuerhalten.
 
4. Abstimmbares Gitterbauelement nach Anspruch 1, mit einer Stromquelle zum Anlegen eines abnehmenden Wechselstroms an den Elektromagneten zum Entfernen einer remanenten Magnetisierung des Paars von Magneten.
 
5. Abstimmbares Gitterbauelement nach Anspruch 1, bei dem die Magnete voneinander beabstandet sind, wobei benachbarte Enden entweder eine entgegengesetzte magnetische Polarität oder die gleiche magnetische Polarität aufweisen.
 
6. Abstimmbares Gitterbauelement nach Anspruch 1, weiterhin mit einer Stromquelle zum Anlegen eines gepulsten Stroms an den Elektromagneten.
 
7. Abstimmbares Gitterbauelement nach Anspruch 1, bei dem die Magnete des Paars eine quadratische Hystereseschleife zum Erzeugen eines Gitterbauelements mit einem bistabilen Wellenlängenverhalten aufweisen.
 
8. Abstimmbares Gitterbauelement nach Anspruch 1, bei dem die Magnete entweder durch eine unmagnetische Verlängerung oder eine Verlängerung aus magnetischem Material, beispielsweise weichmagnetischem Material, an der Faser befestigt sind.
 
9. Abstimmbares Gitterbauelement nach Anspruch 1, bei dem die Faser durch ein unmagnetisches Substrat an einem Magneten des Paars befestigt ist.
 
10. Abstimmbares Gitterbauelement nach Anspruch 1, weiterhin mit einem Rückflußweg, der sich zwischen gegenüberliegenden des Paars von Magnetfeldleckstellen erstreckt.
 
11. Optischer Multiplexer/Demultiplexer mit mindestens einem ersten und einem zweiten optischen Zirkulator (90a, 90b) und einem Gitter einer optischen Faser (12a), das den ersten und den zweiten optischen Zirkulator miteinander verbindet, wobei das faseroptische Gitter ein abstimmbares Gitter nach Anspruch 1 ist.
 
12. Optischer N-Kanal-ADD/DROP-Multiplexer/Demultiplexer mit mehreren optischen Zirkulatoren (90a, 90b, 90c, ...) und mehreren faseroptischen Gittern (12a, 12b, 12c), die durch eine optische Faser verbunden sind, um einen optischen Kommunikationskanal zu der Faser hinzuzufügen oder aus ihr herauszunehmen, wobei mindestens ein faseroptisches Gitter ein abstimmbares Gitter nach Anspruch 1 ist.
 
13. Optisches Wellenlängenmultiplex-Kommunikationssystem, das folgendes umfaßt: eine Quelle (100), eine optische Fernfaser (11) zum Übertragen von optischen Mehrwellen-Signalkanälen von der Quelle aus; und einen Multiplexer/Demultiplexer, der ein Bauelement nach Anspruch 1 umfaßt.
 


Revendications

1. Dispositif de réseau de fibre optique accordable comprenant :

une longueur de fibre optique (11) comportant un réseau optique (12) le long d'une partie de sa longueur;

une paire d'aimants (14, 15) fixés à ladite fibre sur des côtés opposés dudit réseau ;

un électro-aimant (16, 17) pour appliquer un champ magnétique auxdits aimants, induisant ainsi une force entre lesdits aimants et créant une contrainte aux bornes dudit réseau.


 
2. Dispositif de réseau accordable selon la revendication 1, dans lequel les aimants de ladite paire maintiennent une contrainte rémanente dans ledit réseau jusqu'à la désactivation.
 
3. Dispositif de réseau accordable selon la revendication 1, comportant une source de courant pour activer ledit électro-aimant par une impulsion C.C pour produire une magnétisation rémanente suffisante des aimants de ladite paire en vue de maintenir une contrainte rémanente dans ledit réseau.
 
4. Dispositif de réseau accordable selon la revendication 1, comportant une source de courant pour appliquer un courant C.A. décroissant audit électro-aimant pour supprimer la magnétisation rémanente de ladite paire d'aimants.
 
5. Dispositif de réseau accordable selon la revendication 1, dans lequel lesdits aimants sont espacés avec des extrémités adjacentes ayant soit une polarité magnétique opposée, soit la même polarité magnétique.
 
6. Dispositif de réseau accordable selon la revendication 1, comprenant en outre une source de courant pour appliquer un courant pulsé audit électro-aimant.
 
7. Dispositif de réseau accordable selon la revendication 1, dans lequel les aimants de ladite paire présentent une boucle d'hystérésis carrée pour produire un dispositif de réseau ayant une réponse de longueur d'onde bistable.
 
8. Dispositif de réseau accordable selon la revendication 1, dans lequel lesdits aimants sont fixés à ladite fibre par soit une extension non magnétique, soit une extension de matière magnétique, par exemple une matière magnétique tendre.
 
9. Dispositif de réseau accordable selon la revendication 1, dans lequel ladite fibre est fixée à un aimant de ladite paire à travers un substrat non magnétique.
 
10. Dispositif de réseau accordable selon la revendication 1, comprenant en outre un trajet de retour de flux s'étendant entre l'opposé de ladite paire de fuite de champ magnétique.
 
11. Multiplexeur/démultiplexeur optique comprenant au moins un premier et un deuxième circulateur optique (90a, 90b) et un réseau de fibre optique (12a) connectant ledit premier et ledit deuxième circulateur optique, dans lequel ledit réseau de fibre optique est un réseau accordable selon la revendication 1.
 
12. Multiplexeur/démultiplexeur d'ADDITION/REJET optique à N voies comprenant une pluralité de circulateurs optiques (90a, 90b, 90c,...) et une pluralité de réseaux de fibres optiques (12a, 12b, 12c) interconnectés par une fibre optique pour ajouter et/ou rejeter une voie de communications optique de ladite fibre, dans lequel au moins un réseau de fibre optique est un réseau accordable selon la revendication 1.
 
13. Système de communications optique multiplexé en longueur d'onde comprenant : une source (100) ; une fibre de jonction optique (11) pour l'émission de voies de signaux optiques à longueurs d'onde multiples à partir de ladite source ; et un multiplexeur/démultiplexeur, qui comprend un dispositif selon la revendication 1.
 




Drawing